360 XV NORMED ALGEBRAS AND SPECTRAL THEORY
(15.8.1) Let b be a closed left ideal in A, and put Ub(x) - y = xy for all
y e b and all x e A. Then x\-> Ub(x) is a representation of the algebra A on the
Hilbert space b.
First of all, Ub(x) is a continuous operator on b, by (184.108.40.206). Clearly
Ub(xx') = Ub(x)Ub(xf). For y, z in b, we have
(Ub(x)*-y\z) = (y\Ub(x) • z) = (y\xz) = (x*y\z) = (Ub(x*)-y\z)
by virtue of (220.127.116.11), hence Ub(x)* = Ub(x*). Also if A has a unit element e,
then Ub(e) is the identity transformation.
When b = A, we write U(x) in place of UA(x); the representation U is
called the regular representation of A. It is faithful (1 5.5) by virtue of (1 18.104.22.168).
Moreover, x\-+ U(x) is a continuous linear mapping of A into =2?(A), by the
continuity of (x, y) i-* xy.
The study of complete Hilbert algebras is founded on the consideration of
their minimal left ideals and the idempotents which generate them.
For each left ideal I of A, we denote by I* the image of I under the involu-
tion ^H*,?*; clearly I* is a right ideal.
(15.8.2) For each left ideal I of A, the orthogonal supplement I1 of the closure
I 0/1 is a left ideal.
Since I is a left ideal (15.1.3), we may as well assume that I is closed. If
y e I1 and z e A, then for each x e I we have (zy \ x) = (y \ z*x) = 0 because I is
a left ideal, whence it follows that zy e I1.
(15.8.3) Lete^Q be an idempotent in A. Then
(ii) e* is idempotent ;
(iii) the left ideal Ae is the set of all x e A such that x = xe, and is
closed in A.
The first assertion follows from the inequality ||i|| = \\e2\\ ^ \\e\\2. The
second is trivial. As to (iii), it is clear that if x = xe then x e Ae, and conversely
if x e Ae, then x = ye for some y e A, hence xe = ye2 = ye = x. The fact that
Ae is closed then follows from the continuity of the mapping xt~+x — xe,
and (3.1 5.1).
Consider in particular the self-adjoint idempotents (cf. (22.214.171.124 )):
(15.8.4) Ifel9 e2 are self-adjoint idempotents in A, then the following proper-
ties are equivalent: (a) (e± \e2) = 0; (b) e±e2 == 0; (c) e2 et = 0.te Hilbert algebra.